FE Civil exam practice: cram pack

Formula sheets, the key method steps for every topic and 30 practice problems, with full solutions at the back.

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1Formulas and methods

Beam support reactions

Equilibrium
ΣFx = 0, ΣFy = 0, ΣM = 0
Uniform load
resultant w·L at the middle of the load
Moment
M = F·d

Method

  1. Draw a free-body diagram and replace each support by its reactions.
  2. Replace every distributed load by a single force at its centroid.
  3. Take moments about one support to find the reaction at the other.
  4. Use ΣFy = 0 to find the remaining reaction, and check with a second moment equation.

Truss: method of joints

Method of joints
ΣFx = 0, ΣFy = 0 at each joint
Method of sections
ΣM = 0 about a cut point
Member force
positive = tension, negative = compression

Method

  1. Find the support reactions for the whole truss.
  2. Method of joints: start at a joint with at most two unknown member forces and use ΣFx = 0 and ΣFy = 0.
  3. Method of sections: cut through the member you need and take moments about a point where the other unknown members meet.
  4. Assume tension; a negative answer means compression.

Shear force & bending moment

Shear and moment
V = ΣF on one side, M = ΣF·d on one side
Bending stress
σ = M·y/I
Rectangle
I = bh³/12
Section modulus
W = I/ymax
Simply supported, uniform load
Mmax = wL²/8

Method

  1. Find the support reactions from equilibrium of the whole beam.
  2. Cut the beam at the section you need and keep one side.
  3. Shear force: sum of the vertical forces on that side. Bending moment: sum of their moments about the cut.
  4. For the maximum moment, find where the shear force is zero.

Beam deflection

Point load at midspan
δ = PL³/(48EI)
Uniform load, simply supported
δ = 5wL⁴/(384EI)
Cantilever, end load
δ = PL³/(3EI)
Cantilever, uniform load
δ = wL⁴/(8EI)
Superposition
δ = δ1 + δ2

Column buckling

Euler load
Pcr = π²EI/(KL)²
Effective length factor
K = 1 pinned–pinned, 0.5 fixed–fixed, 0.7 fixed–pinned, 2 fixed–free
Critical stress
σcr = Pcr/A
Slenderness
λ = KL/r, r = √(I/A)

Centroid & second moment of area

Centroid
ȳ = ΣAiyi/ΣAi
Rectangle
I = bh³/12
Parallel-axis theorem
I = Ic + A·d²
Composite section
I = Σ(Ic,i + Aidi²)

Effective stress in soil

Total stress
σ = Σγi·hi
Pore water pressure
u = γw·(z − zw)
Effective stress
σ′ = σ − u
Water
γw = 9.81 kN/m³

Consolidation settlement

Normally consolidated
S = Cc·H/(1 + e0)·log₁₀(σ′f/σ′0)
Final stress
σ′f = σ′0 + Δσ (at mid-depth of the layer)
Overconsolidated, σ′f ≤ σ′p
S = Cr·H/(1 + e0)·log₁₀(σ′f/σ′0)
Overconsolidated, σ′f > σ′p
S = H/(1 + e0)·[Cr·log₁₀(σ′p/σ′0) + Cc·log₁₀(σ′f/σ′p)]
Overconsolidation ratio
OCR = σ′p/σ′0
Time for consolidation
t = Tv·Hdr²/cv
Drainage path
Hdr = H/2 (double drainage), H (single drainage)
Time factors
U 50% → 0.197, 60% → 0.287, 70% → 0.403, 80% → 0.567, 90% → 0.848

Hydrostatic force

Pressure at depth
p = ρgh
Force on a vertical wall
F = ρg·hc·A
Centre of pressure
yp = yc + Ic/(ycA)
Rectangle
Ic = bH³/12

Pipe friction & head loss

Reynolds number
Re = V·D/ν = ρ·V·D/μ
Flow regime
laminar below Re ≈ 2000, turbulent above Re ≈ 4000
Mean velocity
V = Q/A, A = π·D²/4
Darcy–Weisbach
hf = f·(L/D)·V²/(2g)
Minor losses
hm = ΣK·V²/(2g)
Typical K values
entrance 0.5, exit 1.0, 90° bend ≈ 0.3
Pressure drop
Δp = ρ·g·hf
Two open reservoirs
Δz = (f·L/D + ΣK)·V²/(2g)
Free outlet
H = (1 + f·L/D + ΣK)·V²/(2g)

Open-channel flow (Manning)

Manning equation
V = (1/n)·R2/3·S1/2
Flow rate
Q = A·V
Hydraulic radius
R = A/P (P = wetted perimeter, free surface excluded)
Rectangle
A = b·y, P = b + 2y
Trapezoid (side slope z:1)
A = (b + z·y)·y, P = b + 2y·√(1 + z²)
Circular pipe, full or half full
R = D/4
Required slope
S = (n·Q/(A·R2/3))²

Pumps & pump power

Hydraulic power
Ph = ρ·g·Q·H = Q·Δp
Shaft power
Pshaft = Ph/ηpump
Electrical power
Pel = Pshaft/ηmotor
Pump head
H = Δz + Δp/(ρ·g) + hL
System losses
hL = (f·L/D + ΣK)·V²/(2g)

Time value of money

Future value
FV = PV·(1 + i)n
Present value
PV = FV/(1 + i)n
Several periods per year
i = r/m, N = m·n
Annuity, present value
PV = PMT·[1 − (1 + i)−n]/i
Annuity, future value
FV = PMT·[(1 + i)n − 1]/i

Method

  1. Draw a timeline with every cash flow and its timing.
  2. Match the rate to the period: a monthly rate for monthly payments.
  3. Use FV = PV·(1 + i)ⁿ for single amounts and the annuity formulas for equal payments.
  4. Check the sign and the order of magnitude of the answer.

NPV & IRR

Net present value
NPV = −C0 + Σ CFt/(1 + r)t
Equal cash flows
NPV = −C0 + CF·[1 − (1 + r)−n]/r
Internal rate of return
the r at which NPV = 0
Decision
accept when NPV > 0 (or IRR > required return)

Method

  1. List all cash flows with their year; the investment at year 0 is negative.
  2. Discount each cash flow: CFt/(1 + r)t.
  3. Add them up to get the NPV. Positive means the project earns more than r.
  4. For the IRR, find the rate that makes NPV zero by trial or interpolation.

Normal distribution

z-score
z = (x − μ)/σ
Below x
P(X < x) = Φ(z)
Above x
P(X > x) = 1 − Φ(z)
Between
Φ(z2) − Φ(z1)
Percentile
x = μ + z·σ

Method

  1. Convert the value to a z-score: z = (x − μ)/σ.
  2. Look up Φ(z), the area to the left of z.
  3. For the area to the right use 1 − Φ(z); for an interval subtract the two left areas.
  4. For a percentile, work backwards: find z for the area, then x = μ + z·σ.

2Practice problems

1.Beam support reactionsMedium
P1​ = 45 kNP2​ = 35 kNABRA​ = ?RB​2 m2 m1 m

The simply supported beam has a pin at A and a roller at B. Find the vertical support reaction RA.

L = 5 mP1 = 45 kN at 2 mP2 = 35 kN at 4 m
RA = kN
2.Beam support reactionsHard
P = 30 kN, 60°Q = 40 kNABRA​ = ?2.5 m2 m1.5 m

The simply supported beam has a pin at A and a roller at B. A load P acts at 2.5 m from A, inclined at 60° to the horizontal, and a vertical load Q acts at 4.5 m from A. Find the magnitude of the total reaction force RA at the pin A.

L = 6 mP = 30 kN at 2.5 m, θ = 60°Q = 40 kN at 4.5 m
RA = kN
3.Truss: method of jointsMedium
ABBCACACB25 kN5 m2 m3 m

Use the method of joints to find the force FBC in member BC. Give tension as positive and compression as negative.

span = 5 mheight = 3 mB is 2 m from Avertical load = 25 kN
FBC = kN
4.Truss: method of jointsHard
ABBCACACB50 kN15 kN6 m5 m2 m

Use the method of joints to find the force FAC in member AC. Give tension as positive and compression as negative.

span = 6 mheight = 2 mB is 5 m from Avertical load = 50 kNhorizontal load = 15 kN →
FAC = kN
5.Shear force & bending momentMedium
w = 5 kN/mABsection4.5 m5.5 m

Find the bending moment Mx at the section x = 4.5 m from support A. Use sagging moments positive and upward shear on the left face positive.

L = 10 mw = 5 kN/m from 0 to 10 mx = 4.5 m
Mx = kN·m
6.Shear force & bending momentHard
8 kN/m15 kN15 kNABCDEFG2 m2 m2 m2 m2 m2 m

The marks A to G split the beam into six equal parts. At which mark is the bending moment largest in size, sagging or hogging? Click it in the diagram.

15 kN @ 0 m15 kN @ 12 m8 kN/m, 2–10 m
  1. 1A (x = 0 m)
  2. 2B (x = 2 m)
  3. 3C (x = 4 m)
  4. 4D (x = 6 m)
  5. 5E (x = 8 m)
  6. 6F (x = 10 m)
  7. 7G (x = 12 m)
7.Beam deflectionMedium
P = 21 kNABδ2.5 m1.5 m

A simply supported beam carries a point load P at a = 2.5 m from support A. Find the deflection δP under the load.

P = 21 kNa = 2.5 mL = 4 mE = 200 GPa (steel)I = 12 × 10⁶ mm⁴
δP = mm
8.Beam deflectionHard
w = 4 kN/mABδ4 m

A simply supported timber beam of rectangular section, 100 mm wide, carries a uniformly distributed load w over its whole span. Its midspan deflection may not exceed span/250. Find the smallest depth hreq of the section.

w = 4 kN/mL = 4 mE = 11 GPa (timber)b = 100 mm
hreq = mm
9.Column bucklingMedium
PL = 4 m30 × 100 mmcross-section

A column of length L made of aluminium is fixed at the base and pinned at the top. Using Euler’s formula, find its critical buckling load Pcr.

L = 4 mE = 70 GPa (aluminium)b × h = 30 × 100 mm
Pcr = kN
10.Column bucklingHard
P = 130 kNL = 2.5 md = ?cross-section

A solid round column of length L made of steel is pinned at both ends. It must carry 130 kN with a factor of safety of 2.5 against buckling. Find the smallest diameter d.

P = 130 kNn = 2.5L = 2.5 mE = 200 GPa (steel)
d = mm
11.Centroid & second moment of areaMedium
1502801612xdimensions in mm

A symmetric I-section has flanges 150 mm wide and 16 mm thick, an overall depth of 280 mm and a web 12 mm thick. Find its elastic section modulus Sx for bending about the horizontal centroidal axis x.

B = 150 mmH = 280 mmtf = 16 mmtw = 12 mm
Sx = × 10³ mm³
12.Centroid & second moment of areaHard
150 mm200 mm120 mm50 × 40xIx​ = ?

A 150 mm × 200 mm plate has a rectangular cut-out 50 mm wide and 40 mm high, centred on the vertical centre line with its centre 120 mm above the bottom. Find the second moment of area Ix about the horizontal axis through the centroid.

b = 150 mmh = 200 mmcut-out: 50 × 40 mmhole centre: y = 120 mm
Ix = × 10⁶ mm⁴
13.Effective stress in soilMedium
sandγd​ = 16.5 kN/m³γsat​ = 19 kN/m³7 mwater tableXz = 7 m

For the soil profile shown, find the vertical effective stress σ′ at point X.

z = 7 mzw = 4 mγw = 9.81 kN/m³sand: γd = 16.5 kN/m³sand: γsat = 19 kN/m³
σ′ = kPa
14.Effective stress in soilHard
sandγd​ = 15 kN/m³γsat​ = 20 kN/m³4 mclayγsat​ = 18 kN/m³5 mwater tableXz = 6.5 m

For the soil profile shown, find the vertical effective stress σ′ at point X.

z = 6.5 mzw = 3 mγw = 9.81 kN/m³sand: γd = 15 kN/m³sand: γsat = 20 kN/m³clay: γsat = 18 kN/m³
σ′ = kPa
15.Consolidation settlementMedium
Δσ = 80 kPasandclayCc​ = 0.3, Cr​ = 0.06e0​ = 0.95σ′0​ = 110 kPaσ′p​ = 140 kPa7 mwater table

A 7 m thick overconsolidated clay layer has Cc = 0.3, Cr = 0.06 and e₀ = 0.95. At its mid-depth the effective vertical stress is 110 kPa and the preconsolidation pressure is 140 kPa. A new building adds 80 kPa of vertical stress at mid-depth. Find the primary consolidation settlement S in mm.

H = 7 mCc = 0.3Cr = 0.06e0 = 0.95σ′0 = 110 kPaσ′p = 140 kPaΔσ = 80 kPa
S = mm
16.Consolidation settlementHard
sandclayH = 7.5 m7.5 msandwater table

In a laboratory oedometer test, a clay specimen 25 mm thick, drained at the top and bottom, reaches 50% consolidation in 6 min. In the field the same clay forms a layer 7.5 m thick. It lies between two sand layers, so water drains out at the top and the bottom. How many days t does the field layer take to reach 50% consolidation?

hlab = 25 mmtlab = 6 minH = 7.5 mfield: double drainage
t = days
17.Hydrostatic forceMedium
gated = 2.5 mH = 2.5 m

A vertical rectangular gate 3 m wide sits in the wall of a tank of water, with its top edge 2.5 m below the surface. Find the resultant hydrostatic force F on the gate.

d = 2.5 mH = 2.5 mb = 3 mρ = 1000 kg/m³g = 9.81 m/s²
F = kN
18.Hydrostatic forceHard
gated = 2 mH = 2.5 m

A vertical rectangular gate 2 m wide sits in the wall of a tank of oil, with its top edge 2 m below the surface. Find the depth ycp of the centre of pressure below the surface.

d = 2 mH = 2.5 mb = 2 mρ = 880 kg/m³g = 9.81 m/s²
ycp = m
19.Pipe friction & head lossMedium
Q = 25 L/sD = 100 mmL = 800 mf = 0.028

Water flows at 25 L/s through a pipe 800 m long with an inside diameter of 100 mm. Use the Darcy friction factor f = 0.028 and g = 9.81 m/s². Find the friction head loss hf.

Q = 25 L/sL = 800 mD = 100 mmf = 0.028g = 9.81 m/s²
hf = m
20.Pipe friction & head lossHard
K = 5Δz = 28 mL = 200 m, D = 200 mm, f = 0.0254× bend (K = 0.3)

Two open reservoirs are joined by a pipe 200 m long with an inside diameter of 200 mm and a Darcy friction factor f = 0.025. The water surface of the upper reservoir is 28 m above that of the lower one. The minor losses are a square-edged entrance (K = 0.5), 4 bends (K = 0.3 each), a valve (K = 5) and the exit into the lower reservoir (K = 1.0). Use g = 9.81 m/s². Find the flow rate Q in L/s.

Δz = 28 mL = 200 mD = 200 mmf = 0.025Kentrance = 0.5Kbend = 0.3 (×4)Kvalve = 5Kexit = 1.0
Q = L/s
21.Open-channel flow (Manning)Medium
D = 300 mmn = 0.013, S = 0.002

A concrete storm sewer with an inside diameter of 300 mm flows just full (as an open channel, not under pressure). Manning n = 0.013 and the slope is S = 0.002. Find the flow rate Q in m³/s.

D = 300 mmn = 0.013S = 0.002
Q = m³/s
22.Open-channel flow (Manning)Hard
D = 250 mmn = 0.013, V = 0.9 m/s

A concrete sewer with an inside diameter of 250 mm (Manning n = 0.013) must reach a self-cleansing velocity of 0.9 m/s when flowing just full. Find the minimum slope S (in m/m).

D = 250 mmn = 0.013V = 0.9 m/s
S = m/m
23.Pumps & pump powerMedium
PQ = 100 L/sH = 38 m

A pump delivers 100 L/s of water (ρ = 1000 kg/m³) against a head of 38 m. The pump efficiency is 80% and the electric motor driving it has an efficiency of 95%. Use g = 9.81 m/s². Find the electrical power Pel the motor draws, in kW.

Q = 100 L/sH = 38 mηpump = 80%ηmotor = 95%g = 9.81 m/s²
Pel = kW
24.Pumps & pump powerHard
PQ = 75 L/sΔz = 7 mL = 600 m, D = 200 mm, f = 0.018, ΣK = 5

A pump moves 75 L/s of water (ρ = 1000 kg/m³) from an open lower reservoir to an upper tank whose water surface is 7 m higher. The pipe is 600 m long with an inside diameter of 200 mm and a Darcy friction factor f = 0.018; the minor-loss coefficients add up to ΣK = 5 (entrance and exit included). Use g = 9.81 m/s². Find the head H the pump must add.

Q = 75 L/sΔz = 7 mL = 600 mD = 200 mmf = 0.018ΣK = 5
H = m
25.Time value of moneyMedium
years0123456PV = ?€2 000€2 000€2 000€2 000

An annuity pays €2 000 at the end of each year for 6 years. The interest rate is 10% per year. Find the present value PV of the annuity.

A = €2 000i = 10%n = 6
PV = €
26.Time value of moneyHard
months0123…120€300€300€300FV = ?

You save €300 at the end of every month for 10 years. The account pays 3% per year, compounded monthly. How much have you saved at the end? Find FV.

A = €3003% / 12N = 120
FV = €
27.NPV & IRRMedium
years0123456−40 0006 5006 5006 5006 5006 50012 500

A machine costs €40 000 today. It generates €6 500 at the end of each year for 6 years and can then be sold for €6 000. The cost of capital is 8%. Find the net present value NPV.

C0 = €40 000CF = €6 500S = €6 000n = 6r = 8%
NPV = €
28.NPV & IRRHard
years012−20 00013 50011 500

A project costs €20 000 and returns €13 500, €11 500 at the end of years 1 to 2. Find its internal rate of return IRR in percent.

CF0 = −20 000CF1 = 13 500CF2 = 11 500
IRR = %
29.Normal distributionMedium
105 s99.9 sX + Y?

X is normal with mean 60 s and standard deviation 5 s; Y is independent and normal with mean 45 s and standard deviation 4 s. Find the probability P that X + Y is more than 99.9 s. Round z to two decimals.

μX = 60, σX = 5μY = 45, σY = 4X + Y > 99.9 s
P =
30.Normal distributionHard
0.02 mm0D − d?

Hole diameters D are normal with mean 25.02 mm and standard deviation 0.01 mm. Shaft diameters d are independent and normal with mean 25 mm and standard deviation 0.02 mm. A randomly chosen shaft fits when D − d > 0. Find the probability P that it fits. Round z to two decimals.

hole: μ = 25.02 mm, σ = 0.01 mmshaft: μ = 25 mm, σ = 0.02 mm
P =

3Solutions

1.Beam support reactions

Answer: RA = 34 kN

Static equilibrium: a body at rest has ΣFx = 0, ΣFy = 0 and ΣM = 0 about any point. Taking moments about one support removes that support’s reaction from the equation.

P1​ = 45 kNP2​ = 35 kNABRA​RB​2 m2 m1 m

Free-body diagram

Replace the supports with reaction forces. A roller gives one vertical reaction; with only vertical loads the pin gives one vertical reaction too.

Equilibrium

Moments about A, counter-clockwise positive. Then vertical force balance.

ΣMA = 0: RB·5 = 45·2 + 35·4
RB = 230/5 = 46 kN
ΣFy = 0: RA = 80 − 46 = 34 kN

Answer

RA = 34 kN
2.Beam support reactions

Answer: RA = 29.29 kN

Static equilibrium: a body at rest has ΣFx = 0, ΣFy = 0 and ΣM = 0 about any point. Replace each distributed load by its resultant (its area) acting at the centroid of the load diagram, and take moments about a support to remove that support’s reaction from the equation.

Components of P

Pv = 30·sin 60° = 25.98 kN
Ph = 30·cos 60° = 15 kN

Reactions

ΣMA = 0: RB·6 = 25.98·2.5 + 40·4.5 → RB = 40.83 kN
Ay = 25.98 + 40 − 40.83 = 25.16 kN
Ax = Ph = 15 kN

Resultant at A

RA = √(15² + 25.16²) = 29.29 kN

Answer

RA = 29.29 kN
3.Truss: method of joints

Answer: FBC = −14.14 kN

Method of joints: every pin of a truss is in equilibrium, so ΣFx = 0 and ΣFy = 0 at each joint. Start at a joint with at most two unknown member forces. A negative result means the member is in compression.

ABBCACACB25 kNAy​Cy​

Support reactions

Equilibrium of the whole truss. Moments about A, counter-clockwise positive.

ΣMA = 0: Cy·5 = 25·2 → Cy = 10 kN
ΣFy = 0: Ay = 25 − 10 = 15 kN

Joint C

The roller gives only a vertical reaction, so joint C has just two unknown member forces. Assume both in tension.

sin γ = 3/4.243 = 0.7071, cos γ = 3/4.243 = 0.7071
ΣFy = 0: Cy + FBC·sin γ = 0 → FBC = −10/0.7071 = −14.14 kN

Answer

FBC = −14.14 kN (compression)
4.Truss: method of joints

Answer: FAC = 23.33 kN

Method of joints: every pin of a truss is in equilibrium, so ΣFx = 0 and ΣFy = 0 at each joint. Start at a joint with at most two unknown member forces. A negative result means the member is in compression.

ABBCACACB50 kN15 kNAy​Cy​Ax​

Support reactions

Equilibrium of the whole truss. Moments about A, counter-clockwise positive.

ΣMA = 0: Cy·6 = 50·5 + 15·2 → Cy = 46.67 kN
ΣFy = 0: Ay = 50 − 46.67 = 3.333 kN
ΣFx = 0: Ax = −15 kN

Joint C

The roller gives only a vertical reaction, so joint C has just two unknown member forces. Assume both in tension.

sin γ = 2/2.236 = 0.8944, cos γ = 1/2.236 = 0.4472
ΣFy = 0: Cy + FBC·sin γ = 0 → FBC = −46.67/0.8944 = −52.17 kN
ΣFx = 0: −FAC − FBC·cos γ = 0 → FAC = −(−52.17)·0.4472 = 23.33 kN

Answer

FAC = 23.33 kN (tension)
5.Shear force & bending moment

Answer: Mx = 61.88 kN·m

Method of sections: cut the beam where you want the internal forces and keep one side. The shear force V balances the vertical forces on that side, and the bending moment M balances their moments about the cut.

Support reactions

Equilibrium of the whole beam.

UDL resultant: W = w·ℓ = 5·10 = 50 kN, acting at x̄ = 5 m
ΣMA = 0: RB·10 = 5·10·5
RB = 250/10 = 25 kN
ΣFy = 0: RA = 50 − 25 = 25 kN
w = 5 kN/mABRA​ = 25RB​ = 25section4.5 m5.5 m

Cut at x = 4.5 m and keep the left part

Only forces left of the cut appear. A UDL portion acts as one force at the middle of that portion.

M = RA·x − (each load left of the cut × its distance to the cut)
Mx = 25·4.5 − 5·4.5·2.25 = 61.88 kN·m

Answer

Mx = 61.88 kN·m
6.Shear force & bending moment

Answer: D (x = 6 m)

Largest bending moment: M changes slope wherever the shear force changes, so its peaks sit where the shear force crosses zero: under a point load, inside a distributed load, or over a support of an overhang. At a fixed support of a cantilever the moment is largest at the wall. Compare the size of M at those places, sagging or hogging.

Support reactions

Take moments about one support, then use the vertical force balance.

R1 = 47 kN, R2 = 47 kN

Bending moment at every mark

Sum the moments of all forces on one side of the cut. Sagging is positive, hogging negative.

MA = 0, MB = −30, MC = 18, MD = 34 kN·m, ME = 18, MF = −30, MG = 0

Answer

Mark D: MD = 34 kN·m
7.Beam deflection

Answer: δP = 10.25 mm

Beam deflection: deflections come from integrating the curvature M/(EI) twice. Standard cases are tabulated, for example PL³/(3EI) for a cantilever with an end load and 5wL⁴/(384EI) for a simply supported beam under a full uniform load. Deflections from separate loads add (superposition).

Consistent units

Work in N and mm: P in N, w in N/mm (kN/m = N/mm), L in mm, E in N/mm² (GPa × 1000), I in mm⁴.

P = 21000 N, a = 2500 mm, b = 1500 mm, L = 4000 mm
EI = 2.4 × 10¹² N·mm²

Deflection under the load

δP = Pa²b²/(3EIL) = 21000·2500²·1500²/(3·2.4 × 10¹²·4000) = 10.25 mm

Answer

δP = 10.25 mm
8.Beam deflection

Answer: hreq = 208.7 mm

Beam deflection: deflections come from integrating the curvature M/(EI) twice. Standard cases are tabulated, for example PL³/(3EI) for a cantilever with an end load and 5wL⁴/(384EI) for a simply supported beam under a full uniform load. Deflections from separate loads add (superposition).

Consistent units

Work in N and mm: P in N, w in N/mm (kN/m = N/mm), L in mm, E in N/mm² (GPa × 1000), I in mm⁴.

w = 4 N/mm, L = 4000 mm, E = 11000 N/mm²

Deflection limit

δallow = L/250 = 4000/250 = 16 mm

Required second moment of area

Ireq = 5wL⁴/(384·E·δallow) = 5·4·4000⁴/(384·11000·16) = 7.576 × 10⁷ mm⁴

Required depth

bh³/12 = Ireq → h = (12·7.576 × 10⁷/100)1/3 = 208.7 mm

Answer

hreq = 208.7 mm

In practice, choose the next standard depth above this value.

9.Column buckling

Answer: Pcr = 19.83 kN

Euler buckling: a slender column becomes unstable at Pcr = π²EI/(KL)², where KL is the effective length: K = 1 for pinned–pinned, 2 for fixed–free, 0.7 for fixed–pinned and 0.5 for fixed–fixed. It buckles about the axis with the smallest I. The formula holds for slender columns, whose critical stress stays below the yield stress.

Smallest second moment of area

A rectangle buckles about its weak axis, using the smaller dimension cubed.

Imin = h·b³/12 = 100·30³/12 = 225000 mm⁴

Effective length

KL = 0.7·4000 = 2800 mm

Critical load

Pcr = π²EI/(KL)² = π²·70000·225000/2800² = 19827 N = 19.83 kN

Answer

Pcr = 19.83 kN
10.Column buckling

Answer: d = 67.67 mm

Euler buckling: a slender column becomes unstable at Pcr = π²EI/(KL)², where KL is the effective length: K = 1 for pinned–pinned, 2 for fixed–free, 0.7 for fixed–pinned and 0.5 for fixed–fixed. It buckles about the axis with the smallest I. The formula holds for slender columns, whose critical stress stays below the yield stress.

Required critical load

Pcr = n·P = 2.5·130000 = 325000 N
KL = 1·2500 = 2500 mm

Solve for the diameter

d = (64·n·P·(KL)²/(π³E))^(1/4) = (64·325000·2500²/(π³·200000))^(1/4) = 67.67 mm

Answer

d = 67.67 mm

Check: the slenderness KL/r is 147.8, so the column is slender and Euler applies.

11.Centroid & second moment of area

Answer: Sx = 707.1 × 10³ mm³

Second moment of area: for a rectangle about its own centroidal axis I = bh³/12, and about its base bh³/3 (parallel-axis theorem I = Ic + A·d²). A hole is handled by subtracting its I, as long as both parts share the same axis. The elastic section modulus is S = I/c, where c is the distance to the extreme fibre.

Outer rectangle minus the two side cut-outs

Both cut-outs together are (B − tw) wide and hw = H − 2tf high, and share the axis x.

hw = 280 − 2·16 = 248 mm
Ix = (B·H³ − (B − tw)·hw³)/12 = (150·280³ − 138·248³)/12
Ix = 9.899 × 10⁷ mm⁴

Section modulus

c = H/2 = 140 mm
Sx = I/c = 9.899 × 10⁷/140
Sx = 707076 mm³ = 707.1 × 10³ mm³

Answer

Sx = 707.1 × 10³ mm³
12.Centroid & second moment of area

Answer: Ix = 98.88 × 10⁶ mm⁴

Sections with holes: treat a hole as a negative area. The centroid is ȳ = (A₁y₁ − A₂y₂)/(A₁ − A₂), with A₁, y₁ for the full plate and A₂, y₂ for the hole. For the second moment of area about the centroidal axis, use the parallel-axis theorem for each part and subtract the hole: I = (Ic1 + A₁d₁²) − (Ic2 + A₂d₂²), where d is the distance from each part's own centroid to the axis through ȳ. A rectangle has Ic = bh³/12 and a circle Ic = πd⁴/64.

Centroid

ȳ = (30000·100 − 2000·120)/(30000 − 2000) = 98.57 mm

Full plate about ȳ

150·200³/12 + 30000·1.429² = 100.1 × 10⁶ mm⁴

Hole about ȳ

50·40³/12 + 2000·21.43² = 1.185 × 10⁶ mm⁴

Subtract

Ix = 98.88 × 10⁶ mm⁴

Answer

Ix = 98.88 × 10⁶ mm⁴
13.Effective stress in soil

Answer: σ′ = 93.57 kPa

Effective stress (Terzaghi): the soil skeleton carries σ′ = σ − u. The total stress σ is the weight of everything above the point, Σγ·h, using the dry unit weight above the water table and the saturated unit weight below it. Below the water table the pore water pressure is hydrostatic: u = γw·(depth below the water table).

Total stress

Add the weight of each soil band above X. Above the water table use the dry unit weight, below it the saturated one.

σ = γd·zw + γsat·(z − zw) = 16.5·4 + 19·3 = 123 kPa

Pore water pressure

Water pressure grows with depth below the water table.

u = γw·(z − zw) = 9.81·3 = 29.43 kPa

Effective stress

σ′ = σ − u = 123 − 29.43 = 93.57 kPa

Answer

σ′ = 93.57 kPa
14.Effective stress in soil

Answer: σ′ = 75.66 kPa

Effective stress (Terzaghi): the soil skeleton carries σ′ = σ − u. The total stress σ is the weight of everything above the point, Σγ·h, using the dry unit weight above the water table and the saturated unit weight below it. Below the water table the pore water pressure is hydrostatic: u = γw·(depth below the water table).

Total stress

Add the weight of each soil band above X. Above the water table use the dry unit weight, below it the saturated one.

σ = γd·3 + γsat,sand·1 + γsat,clay·2.5
σ = 15·3 + 20·1 + 18·2.5 = 110 kPa

Pore water pressure

Water pressure grows with depth below the water table.

u = γw·(z − zw) = 9.81·3.5 = 34.34 kPa

Effective stress

σ′ = σ − u = 110 − 34.34 = 75.66 kPa

Answer

σ′ = 75.66 kPa
15.Consolidation settlement

Answer: S = 165.4 mm

Primary consolidation of a clay layer of thickness H, using the effective stress at the middle of the layer: σ′f = σ′0 + Δσ. Normally consolidated clay: S = Cc·H/(1 + e0)·log₁₀(σ′f/σ′0). Overconsolidated clay recompresses along Cr up to the preconsolidation pressure σ′p and follows Cc only beyond it. Time: t = Tv·Hdr²/cv, where the drainage path Hdr is H/2 when water can leave at the top and bottom, and H when only one side drains.

Compare with the preconsolidation pressure

σ′f = 110 + 80 = 190 kPa > 140 kPa

Settlement

Recompression up to σ′p, virgin compression beyond it.

S = 0.06·7/(1 + 0.95)·log₁₀(140/110) + 0.3·7/(1 + 0.95)·log₁₀(190/140)
S = 22.56 + 142.8 = 165.4 mm

Answer

S = 165.4 mm
16.Consolidation settlement

Answer: t = 375 days

Primary consolidation of a clay layer of thickness H, using the effective stress at the middle of the layer: σ′f = σ′0 + Δσ. Normally consolidated clay: S = Cc·H/(1 + e0)·log₁₀(σ′f/σ′0). Overconsolidated clay recompresses along Cr up to the preconsolidation pressure σ′p and follows Cc only beyond it. Time: t = Tv·Hdr²/cv, where the drainage path Hdr is H/2 when water can leave at the top and bottom, and H when only one side drains.

Drainage paths

Hdr,lab = 25/2 = 12.5 mm = 0.0125 m
Hdr,field = 7.5/2 = 3.75 m

Scale the time

t = Tv·Hdr²/cv with the same T_v and cv in the lab and the field.

tfield = 6·(3.75/0.0125)² = 540000 min
tfield = 540000/1440 = 375 days

Answer

t = 375 days
17.Hydrostatic force

Answer: F = 275.9 kN

Hydrostatic force on a plane surface: F = ρ·g·yc·A. It acts at the centre of pressure, ycp = yc + Ic/(ycA), which always lies below the centroid.

Centroid depth and area

yc = d + H/2 = 2.5 + 2.5/2 = 3.75 m
A = H·b = 2.5·3 = 7.5 m²
gated = 2.5 mH = 2.5 mF

Resultant force

F = ρ·g·yc·A = 1000·9.81·3.75·7.5 = 275.9 kN

Answer

F = 275.9 kN
18.Hydrostatic force

Answer: ycp = 3.41 m

Hydrostatic force on a plane surface: F = ρ·g·yc·A. It acts at the centre of pressure, ycp = yc + Ic/(ycA), which always lies below the centroid.

Centroid depth and area

yc = d + H/2 = 2 + 2.5/2 = 3.25 m
A = H·b = 2.5·2 = 5 m²
gated = 2 mH = 2.5 mF

Resultant force

F = ρ·g·yc·A = 880·9.81·3.25·5 = 140.3 kN

Centre of pressure

Pressure grows with depth, so the resultant acts below the centroid.

Ic = b·H³/12 = 2·2.5³/12 = 2.604 m⁴
ycp = yc + Ic/(yc·A) = 3.25 + 2.604/(3.25·5) = 3.41 m

Answer

ycp = 3.41 m
19.Pipe friction & head loss

Answer: hf = 115.7 m

Pipe flow: the Reynolds number Re = V·D/ν = ρ·V·D/μ tells laminar flow (Re below about 2000) from turbulent flow (above about 4000). Friction along a pipe costs the Darcy–Weisbach head loss hf = f·(L/D)·V²/(2g). Fittings, valves, the entrance and the exit add minor losses hm = ΣK·V²/(2g). Between two open reservoir surfaces the energy equation gives Δz = hf + hm, with the exit loss K = 1 included.

Mean velocity

A = π·0.1²/4 = 0.007854 m²
V = Q/A = 0.025/0.007854 = 3.183 m/s

Velocity head

V²/(2g) = 3.183²/(2·9.81) = 0.5164 m

Darcy–Weisbach

hf = f·(L/D)·V²/(2g) = 0.028·(800/0.1)·3.183²/(2·9.81) = 115.7 m

Answer

hf = 115.7 m
20.Pipe friction & head loss

Answer: Q = 128.8 L/s

Pipe flow: the Reynolds number Re = V·D/ν = ρ·V·D/μ tells laminar flow (Re below about 2000) from turbulent flow (above about 4000). Friction along a pipe costs the Darcy–Weisbach head loss hf = f·(L/D)·V²/(2g). Fittings, valves, the entrance and the exit add minor losses hm = ΣK·V²/(2g). Between two open reservoir surfaces the energy equation gives Δz = hf + hm, with the exit loss K = 1 included.

Loss coefficients

f·L/D = 0.025·200/0.2 = 25
ΣK = 0.5 + 4·0.3 + 5 + 1.0 = 7.7

Energy equation

Both surfaces are open to the air and practically at rest, so all of Δz is lost in the pipe.

28 = (25 + 7.7)·V²/(2·9.81)
V = √(2·9.81·28/32.7) = 4.099 m/s

Flow rate

Q = V·π·D²/4 = 4.099·0.03142 = 0.1288 m³/s = 128.8 L/s

Answer

Q = 128.8 L/s
21.Open-channel flow (Manning)

Answer: Q = 0.04325 m³/s

Manning’s equation (SI): for uniform flow in an open channel V = (1/n)·R2/3·S1/2 and Q = A·V, with n the roughness coefficient, S the bed slope (m/m) and R = A/P the hydraulic radius: flow area divided by wetted perimeter. Only the boundary in contact with the water counts in P, not the free surface. Rectangle: A = b·y, P = b + 2y. Trapezoid with side slopes z:1 (horizontal:vertical): A = (b + z·y)·y, P = b + 2y·√(1 + z²). A circular pipe flowing full or half full has R = D/4.

Geometry

A = 0.07069 m², R = D/4 = 0.075 m

Velocity

V = (1/0.013)·0.0752/3·0.0021/2 = 0.6118 m/s

Flow rate

Q = A·V = 0.07069·0.6118 = 0.04325 m³/s

Answer

Q = 0.04325 m³/s
22.Open-channel flow (Manning)

Answer: S = 0.005519 m/m

Manning’s equation (SI): for uniform flow in an open channel V = (1/n)·R2/3·S1/2 and Q = A·V, with n the roughness coefficient, S the bed slope (m/m) and R = A/P the hydraulic radius: flow area divided by wetted perimeter. Only the boundary in contact with the water counts in P, not the free surface. Rectangle: A = b·y, P = b + 2y. Trapezoid with side slopes z:1 (horizontal:vertical): A = (b + z·y)·y, P = b + 2y·√(1 + z²). A circular pipe flowing full or half full has R = D/4.

Hydraulic radius

R = D/4 = 0.25/4 = 0.0625 m

Solve Manning for S

S = (n·V/R2/3)² = (0.013·0.9/0.1575)² = 0.005519

Answer

S = 0.005519

That is a fall of 5.519 m per kilometre.

23.Pumps & pump power

Answer: Pel = 49.05 kW

Pump power: the power given to the water is the hydraulic power Ph = ρ·g·Q·H = Q·Δp. The shaft must deliver more because the pump loses some: Pshaft = Ph/ηpump, and the motor draws Pel = Pshaft/ηmotor. The pump head H follows from the energy equation: static lift + pressure head + all friction and minor losses.

Hydraulic power

Ph = ρ·g·Q·H = 1000·9.81·0.1·38 = 37.28 kW

Shaft power

Pshaft = 37.28/0.8 = 46.6 kW

Electrical power

Pel = 46.6/0.95 = 49.05 kW

Answer

Pel = 49.05 kW
24.Pumps & pump power

Answer: H = 24.14 m

Pump power: the power given to the water is the hydraulic power Ph = ρ·g·Q·H = Q·Δp. The shaft must deliver more because the pump loses some: Pshaft = Ph/ηpump, and the motor draws Pel = Pshaft/ηmotor. The pump head H follows from the energy equation: static lift + pressure head + all friction and minor losses.

Velocity

V = Q/A = 0.075/0.03142 = 2.387 m/s
V²/(2g) = 0.2905 m

Head losses

hL = (f·L/D + ΣK)·V²/(2g) = (54 + 5)·0.2905 = 17.14 m

Pump head

Both surfaces are open and practically at rest, so pressure and velocity terms drop out.

H = Δz + hL = 7 + 17.14 = 24.14 m

Answer

H = 24.14 m
25.Time value of money

Answer: PV = 8711 €

Time value of money: money today is worth more than the same amount later, because it can earn interest. With interest rate i per period, an amount grows as FV = PV·(1 + i)n. A series of equal payments (an annuity) is valued by adding up each payment, which gives the annuity formulas.

Annuity factor

(1 − (1 + i)−n)/i = (1 − 0.5645)/0.1 = 4.355

Present value

PV = 2 000·4.355 = €8 710.52

Answer

PV = €8 710.52
26.Time value of money

Answer: FV = 41922 €

Time value of money: money today is worth more than the same amount later, because it can earn interest. With interest rate i per period, an amount grows as FV = PV·(1 + i)n. A series of equal payments (an annuity) is valued by adding up each payment, which gives the annuity formulas.

Monthly rate and number of deposits

i = 0.03/12 = 0.0025
N = 12·10 = 120

Future value of the deposits

FV = A·((1 + i)N − 1)/i = 300·(1.349 − 1)/0.0025 = €41 922.43

Answer

FV = €41 922.43

You paid in €36 000 yourself; the rest is interest.

27.NPV & IRR

Answer: NPV = −6170 €

Net present value: discount every cash flow back to today with the required rate of return r, then add them up: NPV = Σ CFₜ/(1 + r)ᵗ. A project with NPV > 0 earns more than r and adds value. The internal rate of return (IRR) is the rate at which NPV = 0.

Present value of the yearly cash flows

6 500·4.623 = 30 048.72

Present value of the salvage value

6 000/1.587 = 3 781.02

NPV

NPV = −40 000 + 30 048.72 + 3 781.02 = −€6 170.26

Answer

NPV = −€6 170.26
28.NPV & IRR

Answer: IRR = 16.75 %

Net present value: discount every cash flow back to today with the required rate of return r, then add them up: NPV = Σ CFₜ/(1 + r)ᵗ. A project with NPV > 0 earns more than r and adds value. The internal rate of return (IRR) is the rate at which NPV = 0.

Bracket the IRR

NPV falls as the rate rises, so the IRR lies between a rate with positive NPV and one with negative NPV.

NPV(15%) = 434.78
NPV(20%) = −763.89

Narrow down

Linear interpolation gives a first estimate; repeating it (or a calculator's IRR function) gives the exact rate.

IRR ≈ 15 + 5·434.78/(434.78 − (−763.89)) = 16.81%
exact: NPV(16.75%) = 0 → IRR = 16.75%

Answer

IRR = 16.75%
29.Normal distribution

Answer: P = 0.7881

Sums and differences of normal variables: if X and Y are independent and normal, X + Y and X − Y are normal too. Means add or subtract: E(X ± Y) = μX ± μY. Variances always add, also for a difference: Var(X ± Y) = σX² + σY², so σ = √(σX² + σY²). Standard deviations never add directly. The total of n independent items with the same distribution has mean n·μ and standard deviation σ·√n. Then standardise as usual: z = (x − mean)/σ and read Φ(z).

Distribution of the sum

μ = 105 s, σ = √(5² + 4²) = 6.403 s

Standardise

z = (99.9 − 105)/6.403 = −0.8

Upper tail

P = 1 − Φ(−0.8) = 1 − 0.2119 = 0.7881

Answer

P = 0.7881
30.Normal distribution

Answer: P = 0.8133

Sums and differences of normal variables: if X and Y are independent and normal, X + Y and X − Y are normal too. Means add or subtract: E(X ± Y) = μX ± μY. Variances always add, also for a difference: Var(X ± Y) = σX² + σY², so σ = √(σX² + σY²). Standard deviations never add directly. The total of n independent items with the same distribution has mean n·μ and standard deviation σ·√n. Then standardise as usual: z = (x − mean)/σ and read Φ(z).

Distribution of the difference

μ = 25.02 − 25 = 0.02 mm, σ = 0.02236 mm

Standardise

z = (0 − 0.02)/0.02236 = −0.89

Probability

P = 1 − Φ(−0.89) = 0.8133

Answer

P = 0.8133

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